1 / 26

Naoyuki Kato (1) , Kazuro Hirahara (2) , and Mikio Iizuka (3)

Numerical simulation of seismic cycles at a subduction zone with a laboratory-derived friction law. Naoyuki Kato (1) , Kazuro Hirahara (2) , and Mikio Iizuka (3) (1) Earthquake Research Institute, University of Tokyo (2) Graduate School of Environmental Sciences, Nagoya University

gigi
Download Presentation

Naoyuki Kato (1) , Kazuro Hirahara (2) , and Mikio Iizuka (3)

An Image/Link below is provided (as is) to download presentation Download Policy: Content on the Website is provided to you AS IS for your information and personal use and may not be sold / licensed / shared on other websites without getting consent from its author. Content is provided to you AS IS for your information and personal use only. Download presentation by click this link. While downloading, if for some reason you are not able to download a presentation, the publisher may have deleted the file from their server. During download, if you can't get a presentation, the file might be deleted by the publisher.

E N D

Presentation Transcript

  1. Numerical simulation of seismic cycles at a subduction zone with a laboratory-derived friction law Naoyuki Kato(1), Kazuro Hirahara(2), and Mikio Iizuka(3) (1) Earthquake Research Institute, University of Tokyo (2) Graduate School of Environmental Sciences, Nagoya University (3) Research Organization for Information Science and Technology

  2. Numerical simulation of seismic cycles at a subduction zone with a laboratory-derived friction lawOutline 1. Composite rate- and state-dependent friction law 2. Forecast models for the Tokai earthquake 3. Mechanism of episodic slip events 4. Historical earthquake sequence along the Nankai trough - Future study -

  3. Rate- and state-dependent friction law m=m*+ a ln(V/V*) + b ln(V*q/L) m; friction coefficient V; sliding velocity q; state variable a,b,L, m*,V*; constants dq/dt = 1 - qV/L; slowness law dq/dt = - (qV/L) ln (qV/L); slip law dq/dt = exp(-V/Vc) - (qV/L) ln (qV/L); composite law Vc; constantKato and Tullis (2001)

  4. Simulation results of slide-hold-slide test Simulation results of velocity stepping test Symmetric responses to velocity increases and decreases for the slip and composite laws explain laboratory data Stiffness independent higher healing rates for the slowness and composite laws explain laboratory data Kato and Tullis (2001)

  5. Simulation of stick-slip cycle of a spring-block system The recurrence interval and stress drop are the largest for the composite law. Kato and Tullis (2002)

  6. Model for seismic cycle at the Tokai seismic gap along the Suruga trough, central Japan Seismic moment release of preseismic sliding seismic gap Back slip distribution estimated from GPS data by Sagiya (1999) 2-D model for the Tokai earthquake Kato and Hirasawa (1999) Kato and Tullis (2002)

  7. 3-D model for the Tokai earthquake Strain change (for one day before EQ) Strain (1E-8) Kuroki et al. (2002)

  8. Hamamatsu Episodic strain event near the hypothesized source area of the Tokai earthquake detected by GPS Data from Geographical Survey Institute (http://www.gsi.go.jp) Hamamatsu

  9. Slow slip event beneath the Bungo channel, southwest Japan Hirose et al. (1999) Velocity changes for 3 years in southwest Japan (c) Apr. 1, 1998 - Apr. 1, 1999 (b) Apr. 1, 1997 - Apr. 1, 1998 (a) Apr. 1, 1996 - Apr. 1, 1997 Observed and model horizontal displacement Distribution of estimated fault slip over 10 months Moment magnitude = 6.6 Saiki Misho Saiki Misho

  10. Possible mechanism of episodic slip event on a plate interface For a spring-block model, the ratio of spring stiffness to the critical stiffness kc= (B-A)/L controls sliding mode. (B-A = -dtss/dlnV, L characteristic slip distance) k >> kc → aseismic k～ kc → episodic k << kc → seismic For a finite fault in a uniform elastic medium, the critical fault dimension rc= cGL/(B-A) may be defined, and r/rc controls sliding mode. (c; constant ～ 1,G; rigidity) r >> rc → seismic r～ rc → episodic r << rc → aseismic k

  11. Simulation of slip on a flat fault in an infinite uniform elastic medium A circular patch with negative A-B value is embedded in a uniform fault with positive A-B value. The critical fault radius rc = 4.12 km. The radius r of the negative A-B patch is 3.0 km. r/rc = 0.73 stable Possibly unstable Distribution of A-B (MPa)

  12. Snapshot of distribution of slip velocity ln(V/Vpl) (Vpl; the assumed plate velocity = 4 cm/yr) The negative A-B patch is more strongly locked.

  13. Snapshot of distribution of slip velocity ln(V/Vpl) Time from the last slide = 5.7 years Episodic slip starts in the negative A-B patch.

  14. Snapshot of distribution of slip velocity ln(V/Vpl) Time from the last slide = 13 hours Episodic slip propagates in the negative A-B patch, but the slip is not significantly accelerated.

  15. Snapshot of distribution of slip velocity ln(V/Vpl) Time from the last slide = 32 days Slip is decelerated because the rupture front enters the positive A-B region.

  16. Snapshot of distribution of slip velocity ln(V/Vpl) Time from the last slide = 150 days Very slow slip propagates in the positive A-B region, while healing starts in the negative A-B patch.

  17. Snapshot of distribution of slip velocity ln(V/Vpl) Time from the last slide = 2.2 years The negative A-B patch is strongly locked and the next cycle starts.

  18. Slip history during the entire cycle r = 3 km, rc = 4.12 km A-B = 0.2 MPa at 1-6 A-B = -0.2 MPa at 7-8

  19. Slip history at the aseismic slip event r = 3 km, rc = 4.12 km A-B = 0.2 MPa at 1-6 A-B = -0.2 MPa at 7-8 TIME (days)

  20. Summary of simulation for episodic slip events Aseismic episodic slip event may be simulated for a negative A-B patch with r/rc= 0.73. Episodic events with various time duration may be simulated by varying r/rc-value. The duration of the event decreases with an increase in r/rc. Episodic events may be simulated not only by nonuniform distribution of A-B but also by nonuniformity in the characteristic slip distance L or in the effective normal stress. If the source size and duration of an episodic event are obtained, the value of (B-A)/L may be estimated.

  21. Earthquake Generation and Strong Motion in 3-D Heterogeneous Media Quasi-Static Modeling of Earthquake Cycle Fault Constitutive Law Interaction on and between Faults Wave Propagation in Heterogeneous Media Dynamic Modeling of Earthquake Rupture Simulation and Prediction of Strong Motion Inland Active Fault Interplate Earthquake Fault Frictional Law Plate Subduction Viscoelastic Interaction

  22. In the Earth Simulator Project, we take into consideration heterogeneous viscoelastic structure, a rate- and state-dependent friction, and interactions of many segments of plate boundary and inland active faults. FEM; Iizuka, Poster Solving friction problem; Prabhakar, Poster

  23. NortheastJapan SouthwestJapan Quasi-Static Earthquake Cycle Simulation with GeoFEM 3D-FEM Mesh 750km 1150km 200km No. of Nodes ：11466 No. of Elements：10000 1100km 900km 200km Crust Plate Upper Mantle No. of Nodes ：59400 No. of Elements：54752

More Related